Production of clusters (up to A=10) during the intranuclear cascade phase of spallation reactionsCugnon, Joseph ; ; et alin Proceedings of the Tenth International Topical Meeting on Nuclear Applications of Accelerators (2012) Detailed reference viewed: 8 (3 ULg) The elusiveness of multifragmentation footprints in 1-GeV proton-nucleus reactions; ; Cugnon, Joseph et alin EPJ Web of Conferences (2012), 31 Extensions of the INCL model to light ion induced reactions for medical and space applications; ; Cugnon, Joseph et alin Proceedings of the 13th INTERNATIONAL CONFERENCE ON NUCLEAR REACTION MECHANISMS (2012) Detailed reference viewed: 9 (0 ULg) The Casimir effect and the vacuum energyCugnon, Joseph ![]() in Few-Body Systems (2012), 53(1-2), 181-188 Detailed reference viewed: 6 (1 ULg) A short introduction to spallation reactionsCugnon, Joseph ![]() in Few-Body Systems (2012), 53(1-2), 142-152 Influence of nuclear de-excitation on observables relevant for space explorationMancusi, Davide ; ; Cugnon, Joseph et alin Advances in Space Research (2011), 47(7), 1194-1199 Detailed reference viewed: 7 (1 ULg) Measurement and simulation of the cross sections for nuclide production in 56Fe and natCr targets irradiated with 0.04- to 2.6-GeV protons; ; et al in Physics of Atomic Nuclei (2011), 74(4), 523-536 The cross sections for nuclide production in thin 56Fe and natCr targets irradiated by 0.04-2.6-GeV protons are measured by direct γ spectrometry using two γ spectrometers with the resolutions of 1.8 and ... [more ▼] The cross sections for nuclide production in thin 56Fe and natCr targets irradiated by 0.04-2.6-GeV protons are measured by direct γ spectrometry using two γ spectrometers with the resolutions of 1.8 and 1.7 keV for the 60Co 1332-keV γ line. As a result, 649 yields of radioactive residual product nuclei have been obtained. The 27Al(p, x) 22Na reaction has been used as a monitor reaction. The experimental data are compared with the MCNPX (BERTINI, ISABEL), CEM03. 02, INCL4. 2, INCL4. 5, PHITS, and CASCADE07 calculations. © 2011 Pleiades Publishing, Ltd. [less ▲] Detailed reference viewed: 4 (2 ULg) Verification of high-energy transport codes on the basis of activation data; ; et al in Physical Review. C : Nuclear Physics (2011), 84(6), Nuclide production cross sections measured at the Institute for Theoretical and Experimental Physics (ITEP) for the targets of natCr, 56Fe, natNi, 93Nb, 181Ta, natW, natPb, and 209Bi irradiated by protons ... [more ▼] Nuclide production cross sections measured at the Institute for Theoretical and Experimental Physics (ITEP) for the targets of natCr, 56Fe, natNi, 93Nb, 181Ta, natW, natPb, and 209Bi irradiated by protons with energies from 40 to 2600 MeV were used to estimate the predictive accuracy of several popular high-energy transport codes. A general agreement of the ITEP data with the data obtained by other groups, including the numerous GSI data measured by the inverse kinematics method was found. Simulations of the measured data were performed with the mcnpx (bertini and isabel options), cem03.02, incl4.2+abla, incl4.5+abla07, phits, and cascade.07 codes. Deviation factors between the calculated and experimental cross sections have been estimated for each target and for the whole energy range covered by our measurements. Two-dimensional diagrams of deviation factor values were produced for estimating the predictive power of every code for intermediate, not measured masses of nuclei targets and bombarding energies of protons. Further improvements of all tested here codes are recommended. In addition, new measurements at ITEP of nuclide yields from the 208Pb target irradiated by 500-MeV protons are presented. A good agreement between these new data and the GSI measurements obtained by the inverse kinematics method was found. © 2011 American Physical Society. [less ▲] Detailed reference viewed: 5 (1 ULg) Elusiveness of evidence for multifragmentation in 1-GeV proton-nucleus reactions; ; Cugnon, Joseph et alin Physical Review. C : Nuclear Physics (2011), 84(6), We use the tools of hybrid intranuclear-cascade/nuclear-deexcitation models to evaluate the sensitivity of several physical observables to the inclusion of a multifragmentation stage in the deexcitation ... [more ▼] We use the tools of hybrid intranuclear-cascade/nuclear-deexcitation models to evaluate the sensitivity of several physical observables to the inclusion of a multifragmentation stage in the deexcitation chain and assess the need for a multifragmentation model in the quantitative description of p + 56Fe and p + 136Xe reactions at 1-GeV incident energy. We seek clear signatures of multifragmentation by comparing different state-of-the-art deexcitation models coupled with intranuclear-cascade models and by focusing on discriminating observables such as correlations and fragment longitudinal-velocity distributions. None of the considered observables can be unambiguously interpreted as a multifragmentation footprint. The experimental data are best described as originating from sequential binary decays. However, no deexcitation model can reproduce the experimental longitudinal-velocity distributions from 1-GeV p + 136Xe. © 2011 American Physical Society. [less ▲] Detailed reference viewed: 4 (0 ULg) The photon wave functionCugnon, Joseph ![]() in Open Journal of Microphysics (2011), 1 Detailed reference viewed: 1 (1 ULg) Spallation modeling- What's new on nuclei production with INCL4.5-Abla07?; ; Cugnon, Joseph et alin Memorie della Società Astronomica Italiana (2011), 82(2), 909-912 Detailed reference viewed: 1 (0 ULg) Measurement and simulation of the cross sections for the production of 148Gd in thin natW and 181Ta targets irradiated with 0.4- to 2.6-GeV protons; ; et al in Physics of Atomic Nuclei (2011), 74(4), 573-579 The cross sections for the production of 148Gd in natW and 181Ta targets irradiated by 0.4-, 0.6-, 0.8-, 1.2-, 1.6-, and 2.6-GeV protons at the ITEP accelerator complex have been measured by direct α ... [more ▼] The cross sections for the production of 148Gd in natW and 181Ta targets irradiated by 0.4-, 0.6-, 0.8-, 1.2-, 1.6-, and 2.6-GeV protons at the ITEP accelerator complex have been measured by direct α spectrometry without chemical separation. The experimental data have been compared with the data obtained at other laboratories and with the theoretical simulations of the yields on the basis of the BERTINI, ISABEL, CEM03. 02, INCL4. 2, INCL4. 5, CASCADE07, and PHITS codes. © 2011 Pleiades Publishing, Ltd. [less ▲] Detailed reference viewed: 1 (0 ULg) Measurement and simulation of the cross sections for nuclide production in 93Nb and natNi targets irradiated with 0.04- to 2.6-GeV protons; ; et al in Physics of Atomic Nuclei (2011), 74(4), 537-550 The cross sections for nuclide production in thin 93Nb and natNi targets irradiated by 0.04- to 2.6-GeV protons have been measured by direct γ spectrometry using two γ spectrometers with the resolutions ... [more ▼] The cross sections for nuclide production in thin 93Nb and natNi targets irradiated by 0.04- to 2.6-GeV protons have been measured by direct γ spectrometry using two γ spectrometers with the resolutions of 1.8 and 1.7 keV in the 60Co 1332-keV γ line. As a result, 1112 yields of radioactive residual nuclei have been obtained. The 27Al(p, x) 22Na reaction has been used as a monitor reaction. The experimental data have been compared with the MCNPX (BERTINI, ISABEL), CEM03.02, INCL4.2, INCL4.5, PHITS, and CASCADE07 calculations. © 2011 Pleiades Publishing, Ltd. [less ▲] Measurement and simulation of the cross sections for nuclide production in natW and 181Ta targets irradiated with 0.04- to 2.6-GeV protons; ; et al in Physics of Atomic Nuclei (2011), 74(4), 551-572 The cross sections for nuclide production in thin natWand 181Ta targets irradiated by 0.04-2.6-GeV protons have been measured by direct γ spectrometry using two γ spectrometers with the resolutions of 1.8 ... [more ▼] The cross sections for nuclide production in thin natWand 181Ta targets irradiated by 0.04-2.6-GeV protons have been measured by direct γ spectrometry using two γ spectrometers with the resolutions of 1.8 and 1.7 keV in the 60Co 1332-keV γ line. As a result, 1895 yields of radioactive residual product nuclei have been obtained. The 27Al(p, x) 22Na reaction has been used as a monitor reaction. The experimental data have been compared with the MCNPX (BERTINI, ISABEL), CEM03. 02, INCL4. 2, INCL4. 5, PHITS, and CASCADE07 calculations. © 2011 Pleiades Publishing, Ltd. [less ▲] Detailed reference viewed: 6 (2 ULg) Production of heavy clusters (up to A=10) by coalescence during the intranuclear cascade phase of spallation reactionsCugnon, Joseph ; ; et alin J. Phys: Conf. Ser. (2011), 312 Detailed reference viewed: 9 (1 ULg)![]() INCL4.5 and Abla07 --- Improved versions of the intranuclear cascade (INCL4) and deexcitation (Abla) models; ; Cugnon, Joseph et alin Proceedings to the Shielding Aspects of Accelerators, Targets and Irradiation Facilities 2010 (2011) Detailed reference viewed: 14 (2 ULg) Extension of the Liège intranuclear cascade model at incident energies between 2 and 12 GeV. Aspects of pion production.; Cugnon, Joseph ![]() in Nuclear Physics A (2011), 866 Detailed reference viewed: 2 (1 ULg) INCL Intra-Nuclear Cascade and ABLA De-excitation Models in GEANT4; ; et al in Progress in NUCLEAR SCIENCE and TECHNOLOGY (2011), 2 Detailed reference viewed: 3 (0 ULg) Constraining fission parameters for highly excited compound nuclei; ; Cugnon, Joseph ![]() in Wagemans, C; Wagemans, J; d'Hondt, P (Eds.) Seminar on fission, het Pand (2011) Detailed reference viewed: 10 (3 ULg) Production of heavy clusters (up to A=10) by coalescence during the intranuclear cascade phase of spallation reactionsCugnon, Joseph ; ; et alin J. Phys.: Conf. Ser. (2011), 312 |
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